Method for operating a linear compressor

ABSTRACT

A method for operating a linear compressor is provided. The method includes supplying a motor of the linear compressor with a time varying voltage and estimating a back-EMF of the motor of the linear compressor. The method also includes determining a velocity of the motor of the linear compressor based at least in part on the back-EMF of the motor and calculating a stroke length of the motor of the linear compressor based at least in part on the velocity of the motor.

FIELD OF THE INVENTION

The present subject matter relates generally to linear compressors, such as linear compressors for refrigerator appliances.

BACKGROUND OF THE INVENTION

Certain refrigerator appliances include sealed systems for cooling chilled chambers of the refrigerator appliances. The sealed systems generally include a compressor that generates compressed refrigerant during operation of the sealed systems. The compressed refrigerant flows to an evaporator where heat exchange between the chilled chambers and the refrigerant cools the chilled chambers and food items located therein.

Recently, certain refrigerator appliances have included linear compressors for compressing refrigerant. Linear compressors generally include a piston and a driving coil. The driving coil receives a current that generates a force for sliding the piston forward and backward within a chamber. During motion of the piston within the chamber, the piston compresses refrigerant. Motion of the piston within the chamber is generally controlled such that the piston does not crash against another component of the linear compressor during motion of the piston within the chamber. Such head crashing can damage various components of the linear compressor, such as the piston or an associated cylinder.

While head crashing is preferably avoided, it can be difficult to determine a position of the piston within the chamber. For example, a stroke length of the piston is dependent upon a variety of parameters of the linear compressor, and such parameters can vary. In addition, utilizing a sensor to measure the stroke length of the piston can require sensor wires to pierce a hermetically sealed shell of the linear compressor. Passing the sensor wires through the shell provides a path for contaminants to enter the shell.

Accordingly, a method for determining a stroke length of a motor of a linear compressor would be useful. In particular, a method for determining a stroke length of a motor of a linear compressor without utilizing a sensor, such as a position, velocity or acceleration sensor, to determine translational mechanical states of the motor would be useful.

BRIEF DESCRIPTION OF THE INVENTION

The present subject matter provides a method for operating a linear compressor. The method includes supplying a motor of the linear compressor with a time varying voltage and estimating a back-EMF of the motor of the linear compressor. The method also includes determining a velocity of the motor of the linear compressor based at least in part on the back-EMF of the motor and calculating a stroke length of the motor of the linear compressor based at least in part on the velocity of the motor. Additional aspects and advantages of the invention will be set forth in part in the following description, or may be apparent from the description, or may be learned through practice of the invention.

In a first exemplary embodiment, a method for operating a linear compressor is provided. The method includes providing an electrical dynamic model for a motor of the linear compressor, supplying the motor of the linear compressor with a time varying voltage, estimating a back-EMF of the motor of the linear compressor during the step of supplying using at least the electrical dynamic model for the motor of the linear compressor and a robust integral of the sign of the error feedback, determining a velocity of the motor of the linear compressor based at least in part on the back-EMF of the motor from the step of estimating, and calculating a stroke length of the motor of the linear compressor based at least in part on the velocity of the motor from the step of determining.

In a second exemplary embodiment, a method for operating a linear compressor is provided. The method includes supplying the motor of the linear compressor with a time varying voltage. The motor of the linear compressor is disposed within a hermetic shell of the linear compressor during the step of supplying. The method also includes estimating a back-EMF of the motor of the linear compressor during the step of supplying using a robust integral of the sign of the error feedback, determining a velocity of the motor of the linear compressor based at least in part on the back-EMF of the motor from the step of estimating, and calculating a stroke length of the motor of the linear compressor based at least in part on the velocity of the motor from the step of determining.

These and other features, aspects and advantages of the present invention will become better understood with reference to the following description and appended claims. The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate embodiments of the invention and, together with the description, serve to explain the principles of the invention.

BRIEF DESCRIPTION OF THE DRAWINGS

A full and enabling disclosure of the present invention, including the best mode thereof, directed to one of ordinary skill in the art, is set forth in the specification, which makes reference to the appended figures.

FIG. 1 is a front elevation view of a refrigerator appliance according to an exemplary embodiment of the present subject matter.

FIG. 2 is schematic view of certain components of the exemplary refrigerator appliance of FIG. 1.

FIG. 3 provides a perspective view of a linear compressor according to an exemplary embodiment of the present subject matter.

FIG. 4 provides a side section view of the exemplary linear compressor of FIG. 3.

FIG. 5 provides an exploded view of the exemplary linear compressor of FIG. 4.

FIG. 6 illustrates a method for operating a linear compressor according to an exemplary embodiment of the present subject matter.

FIG. 7 illustrates a method for operating a linear compressor according to another exemplary embodiment of the present subject matter.

FIG. 8 illustrates a method for operating a linear compressor according to an additional exemplary embodiment of the present subject matter.

FIGS. 9, 10 and 11 illustrate exemplary plots of experimental electrical motor parameter estimates.

DETAILED DESCRIPTION

Reference now will be made in detail to embodiments of the invention, one or more examples of which are illustrated in the drawings. Each example is provided by way of explanation of the invention, not limitation of the invention. In fact, it will be apparent to those skilled in the art that various modifications and variations can be made in the present invention without departing from the scope or spirit of the invention. For instance, features illustrated or described as part of one embodiment can be used with another embodiment to yield a still further embodiment. Thus, it is intended that the present invention covers such modifications and variations as come within the scope of the appended claims and their equivalents.

FIG. 1 depicts a refrigerator appliance 10 that incorporates a sealed refrigeration system 60 (FIG. 2). It should be appreciated that the term “refrigerator appliance” is used in a generic sense herein to encompass any manner of refrigeration appliance, such as a freezer, refrigerator/freezer combination, and any style or model of conventional refrigerator. In addition, it should be understood that the present subject matter is not limited to use in appliances. Thus, the present subject matter may be used for any other suitable purpose, such as vapor compression within air conditioning units or air compression within air compressors.

In the illustrated exemplary embodiment shown in FIG. 1, the refrigerator appliance 10 is depicted as an upright refrigerator having a cabinet or casing 12 that defines a number of internal chilled storage compartments. In particular, refrigerator appliance 10 includes upper fresh-food compartments 14 having doors 16 and lower freezer compartment 18 having upper drawer 20 and lower drawer 22. The drawers 20 and 22 are “pull-out” drawers in that they can be manually moved into and out of the freezer compartment 18 on suitable slide mechanisms.

FIG. 2 is a schematic view of certain components of refrigerator appliance 10, including a sealed refrigeration system 60 of refrigerator appliance 10. A machinery compartment 62 contains components for executing a known vapor compression cycle for cooling air. The components include a compressor 64, a condenser 66, an expansion device 68, and an evaporator 70 connected in series and charged with a refrigerant. As will be understood by those skilled in the art, refrigeration system 60 may include additional components, e.g., at least one additional evaporator, compressor, expansion device, and/or condenser. As an example, refrigeration system 60 may include two evaporators.

Within refrigeration system 60, refrigerant flows into compressor 64, which operates to increase the pressure of the refrigerant. This compression of the refrigerant raises its temperature, which is lowered by passing the refrigerant through condenser 66. Within condenser 66, heat exchange with ambient air takes place so as to cool the refrigerant. A fan 72 is used to pull air across condenser 66, as illustrated by arrows A_(C), so as to provide forced convection for a more rapid and efficient heat exchange between the refrigerant within condenser 66 and the ambient air. Thus, as will be understood by those skilled in the art, increasing air flow across condenser 66 can, e.g., increase the efficiency of condenser 66 by improving cooling of the refrigerant contained therein.

An expansion device (e.g., a valve, capillary tube, or other restriction device) 68 receives refrigerant from condenser 66. From expansion device 68, the refrigerant enters evaporator 70. Upon exiting expansion device 68 and entering evaporator 70, the refrigerant drops in pressure. Due to the pressure drop and/or phase change of the refrigerant, evaporator 70 is cool relative to compartments 14 and 18 of refrigerator appliance 10. As such, cooled air is produced and refrigerates compartments 14 and 18 of refrigerator appliance 10. Thus, evaporator 70 is a type of heat exchanger which transfers heat from air passing over evaporator 70 to refrigerant flowing through evaporator 70.

Collectively, the vapor compression cycle components in a refrigeration circuit, associated fans, and associated compartments are sometimes referred to as a sealed refrigeration system operable to force cold air through compartments 14, 18 (FIG. 1). The refrigeration system 60 depicted in FIG. 2 is provided by way of example only. Thus, it is within the scope of the present subject matter for other configurations of the refrigeration system to be used as well.

FIG. 3 provides a perspective view of a linear compressor 100 according to an exemplary embodiment of the present subject matter. FIG. 4 provides a side section view of linear compressor 100. FIG. 5 provides an exploded side section view of linear compressor 100. As discussed in greater detail below, linear compressor 100 is operable to increase a pressure of fluid within a chamber 112 of linear compressor 100. Linear compressor 100 may be used to compress any suitable fluid, such as refrigerant or air. In particular, linear compressor 100 may be used in a refrigerator appliance, such as refrigerator appliance 10 (FIG. 1) in which linear compressor 100 may be used as compressor 64 (FIG. 2). As may be seen in FIG. 3, linear compressor 100 defines an axial direction A, a radial direction R and a circumferential direction C. Linear compressor 100 may be enclosed within a hermetic or air-tight shell (not shown). The hermetic shell can, e.g., hinder or prevent refrigerant from leaking or escaping from refrigeration system 60.

Turning now to FIG. 4, linear compressor 100 includes a casing 110 that extends between a first end portion 102 and a second end portion 104, e.g., along the axial direction A. Casing 110 includes various static or non-moving structural components of linear compressor 100. In particular, casing 110 includes a cylinder assembly 111 that defines a chamber 112. Cylinder assembly 111 is positioned at or adjacent second end portion 104 of casing 110. Chamber 112 extends longitudinally along the axial direction A. Casing 110 also includes a motor mount mid-section 113 and an end cap 115 positioned opposite each other about a motor. A stator, e.g., including an outer back iron 150 and a driving coil 152, of the motor is mounted or secured to casing 110, e.g., such that the stator is sandwiched between motor mount mid-section 113 and end cap 115 of casing 110. Linear compressor 100 also includes valves (such as a discharge valve assembly 117 at an end of chamber 112) that permit refrigerant to enter and exit chamber 112 during operation of linear compressor 100.

A piston assembly 114 with a piston head 116 is slidably received within chamber 112 of cylinder assembly 111. In particular, piston assembly 114 is slidable along a first axis A1 within chamber 112. The first axis A1 may be substantially parallel to the axial direction A. During sliding of piston head 116 within chamber 112, piston head 116 compresses refrigerant within chamber 112. As an example, from a top dead center position, piston head 116 can slide within chamber 112 towards a bottom dead center position along the axial direction A, i.e., an expansion stroke of piston head 116. When piston head 116 reaches the bottom dead center position, piston head 116 changes directions and slides in chamber 112 back towards the top dead center position, i.e., a compression stroke of piston head 116. It should be understood that linear compressor 100 may include an additional piston head and/or additional chamber at an opposite end of linear compressor 100. Thus, linear compressor 100 may have multiple piston heads in alternative exemplary embodiments.

Linear compressor 100 also includes an inner back iron assembly 130. Inner back iron assembly 130 is positioned in the stator of the motor. In particular, outer back iron 150 and/or driving coil 152 may extend about inner back iron assembly 130, e.g., along the circumferential direction C. Inner back iron assembly 130 extends between a first end portion 132 and a second end portion 134, e.g., along the axial direction A.

Inner back iron assembly 130 also has an outer surface 137. At least one driving magnet 140 is mounted to inner back iron assembly 130, e.g., at outer surface 137 of inner back iron assembly 130. Driving magnet 140 may face and/or be exposed to driving coil 152. In particular, driving magnet 140 may be spaced apart from driving coil 152, e.g., along the radial direction R by an air gap AG. Thus, the air gap AG may be defined between opposing surfaces of driving magnet 140 and driving coil 152. Driving magnet 140 may also be mounted or fixed to inner back iron assembly 130 such that an outer surface 142 of driving magnet 140 is substantially flush with outer surface 137 of inner back iron assembly 130. Thus, driving magnet 140 may be inset within inner back iron assembly 130. In such a manner, the magnetic field from driving coil 152 may have to pass through only a single air gap (e.g., air gap AG) between outer back iron 150 and inner back iron assembly 130 during operation of linear compressor 100, and linear compressor 100 may be more efficient than linear compressors with air gaps on both sides of a driving magnet.

As may be seen in FIG. 4, driving coil 152 extends about inner back iron assembly 130, e.g., along the circumferential direction C. Driving coil 152 is operable to move the inner back iron assembly 130 along a second axis A2 during operation of driving coil 152. The second axis may be substantially parallel to the axial direction A and/or the first axis A1. As an example, driving coil 152 may receive a current from a current source (not shown) in order to generate a magnetic field that engages driving magnet 140 and urges piston assembly 114 to move along the axial direction A in order to compress refrigerant within chamber 112 as described above and will be understood by those skilled in the art. In particular, the magnetic field of driving coil 152 may engage driving magnet 140 in order to move inner back iron assembly 130 along the second axis A2 and piston head 116 along the first axis A1 during operation of driving coil 152. Thus, driving coil 152 may slide piston assembly 114 between the top dead center position and the bottom dead center position, e.g., by moving inner back iron assembly 130 along the second axis A2, during operation of driving coil 152.

A piston flex mount 160 is mounted to and extends through inner back iron assembly 130. A coupling 170 extends between piston flex mount 160 and piston assembly 114, e.g., along the axial direction A. Thus, coupling 170 connects inner back iron assembly 130 and piston assembly 114 such that motion of inner back iron assembly 130, e.g., along the axial direction A or the second axis A2, is transferred to piston assembly 114. Piston flex mount 160 defines an input passage 162 that permits refrigerant to flow therethrough.

Linear compressor 100 may include various components for permitting and/or regulating operation of linear compressor 100. In particular, linear compressor 100 includes a controller (not shown) that is configured for regulating operation of linear compressor 100. The controller is in, e.g., operative, communication with the motor, e.g., driving coil 152 of the motor. Thus, the controller may selectively activate driving coil 152, e.g., by supplying current to driving coil 152, in order to compress refrigerant with piston assembly 114 as described above.

The controller includes memory and one or more processing devices such as microprocessors, CPUs or the like, such as general or special purpose microprocessors operable to execute programming instructions or micro-control code associated with operation of linear compressor 100. The memory can represent random access memory such as DRAM, or read only memory such as ROM or FLASH. The processor executes programming instructions stored in the memory. The memory can be a separate component from the processor or can be included onboard within the processor. Alternatively, the controller may be constructed without using a microprocessor, e.g., using a combination of discrete analog and/or digital logic circuitry (such as switches, amplifiers, integrators, comparators, flip-flops, AND gates, field programmable gate arrays (FPGA), and the like) to perform control functionality instead of relying upon software.

Linear compressor 100 also includes a spring assembly 120. Spring assembly 120 is positioned in inner back iron assembly 130. In particular, inner back iron assembly 130 may extend about spring assembly 120, e.g., along the circumferential direction C. Spring assembly 120 also extends between first and second end portions 102 and 104 of casing 110, e.g., along the axial direction A. Spring assembly 120 assists with coupling inner back iron assembly 130 to casing 110, e.g., cylinder assembly 111 of casing 110. In particular, inner back iron assembly 130 is fixed to spring assembly 120 at a middle portion 119 of spring assembly 120.

During operation of driving coil 152, spring assembly 120 supports inner back iron assembly 130. In particular, inner back iron assembly 130 is suspended by spring assembly 120 within the stator or the motor of linear compressor 100 such that motion of inner back iron assembly 130 along the radial direction R is hindered or limited while motion along the second axis A2 is relatively unimpeded. Thus, spring assembly 120 may be substantially stiffer along the radial direction R than along the axial direction A. In such a manner, spring assembly 120 can assist with maintaining a uniformity of the air gap AG between driving magnet 140 and driving coil 152, e.g., along the radial direction R, during operation of the motor and movement of inner back iron assembly 130 on the second axis A2. Spring assembly 120 can also assist with hindering side pull forces of the motor from transmitting to piston assembly 114 and being reacted in cylinder assembly 111 as a friction loss.

FIG. 6 illustrates a method 600 for operating a linear compressor according to an exemplary embodiment of the present subject matter. Method 600 may be used to operate any suitable linear compressor. For example, method 600 may be used to operate linear compressor 100 (FIG. 3). Thus, method 600 is discussed in greater detail below with reference to linear compressor 100. Utilizing method 600 various mechanical and electrical parameters or constants of linear compressor 100 may be established or determined. For example, method 600 may assist with determining or establishing a spring constant of spring assembly 120, a motor force constant of the motor of linear compressor 100, a damping coefficient of linear compressor 100, a resistance of the motor of linear compressor 100, an inductance of the motor of linear compressor 100, a moving mass (such as mass of piston assembly 114 and inner back iron assembly 130) of linear compressor 100, etc. Knowledge of such mechanical and electrical parameters or constants of linear compressor 100 may improve performance or operation of linear compressor 100, as will be understood by those skilled in the art.

At step 610, an electrical dynamic model for the motor of linear compressor 100 is provided. Any suitable electrical dynamic model for the motor of linear compressor 100 may be provided at step 610. For example, the electrical dynamic model for the motor of linear compressor 100 may be

$\frac{i}{t} = {\frac{v_{a}}{L_{i}} - \frac{r_{i}i}{L_{i}} - \frac{\alpha \; \overset{.}{x}}{L_{i}}}$

where

-   -   v_(a) is a voltage across the motor of linear compressor 100;     -   r_(i) is a resistance of the motor of linear compressor 100;     -   i is a current through the motor of linear compressor 100;     -   α is a motor force constant;     -   {dot over (x)} is a velocity of the motor of linear compressor         100; and     -   L_(i) is an inductance of the motor of linear compressor 100.

The electrical dynamic model for the motor of linear compressor 100 includes a plurality of unknown constants. In the example provided above, the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100 includes the resistance of the motor of linear compressor 100 (e.g., the resistance of driving coil 152), the inductance of the motor of linear compressor 100 (e.g., the inductance of driving coil 152), and the motor force constant. Knowledge or accurate estimates of such unknown constants can improve operation of linear compressor 100, e.g., by permitting operation of linear compressor 100 at a resonant frequency without head crashing.

At step 610, the electrical dynamic model for the motor of linear compressor 100 may also be solved for a particular variable, such as di/dt in the example provided above. Thus, as an example, the electrical dynamic model for the motor of linear compressor 100 may be provided in parametric form as

${\varphi \overset{\Delta}{=}{{W\; \theta_{e}\mspace{14mu} {where}\mspace{20mu} W}\overset{\Delta}{=}\left\lbrack {v_{a}\mspace{14mu} - i\mspace{20mu} - \overset{.}{x}} \right\rbrack}};{and}$ $\theta_{e}\overset{\Delta}{=}{\left\lbrack {\frac{1}{L_{i}}\mspace{14mu} \frac{r_{i}}{L_{i}}\mspace{14mu} \frac{\propto}{L_{i}}} \right\rbrack.}$

However, di/dt is difficult to accurately measure or determine. Thus, a filtering technique may be used to account for this signal and provide a useable or implementable signal. In particular, the electrical dynamic model for the motor of linear compressor 100 may be filtered, e.g., with a low-pass filter, to account for this signal. Thus, a filtered electrical dynamic model for the motor of linear compressor 100 may be provided as

Φ_(f)

W _(f)θ_(e).

In alternative exemplary embodiments, the electrical dynamic model for the motor of linear compressor 100 may be solved for {dot over (x)} at step 610. Thus, the electrical dynamic model for the motor of linear compressor 100 may be provided in parametric form as

${\varphi \overset{\Delta}{=}{{W\; \theta_{e}\mspace{14mu} {where}\mspace{14mu} \varphi}\overset{\Delta}{=}\left\lbrack \frac{i}{t} \right\rbrack}};$ ${W\overset{\Delta}{=}\left\lbrack {v_{a}\mspace{14mu} - i\mspace{20mu} - \frac{i}{t}} \right\rbrack};{and}$ $\theta_{e}\overset{\Delta}{=}{\left\lbrack {\frac{1}{\propto}\mspace{14mu} \frac{r_{i}}{\propto}\mspace{14mu} \frac{L_{i}}{\propto}} \right\rbrack.}$

Again, the electrical dynamic model for the motor of linear compressor 100 may be filtered, e.g., to account for di/dt.

At step 620, each unknown constant of the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100 is estimated. For example, a manufacturer of linear compressor 100 may have a rough estimate or approximation for the value of each unknown constant of the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100. Thus, such values of the each unknown constant of the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100 may be provided at step 620 to estimate each unknown constant of the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100.

At step 630, the motor (e.g., driving coil 152) of linear compressor 100 is supplied with a time varying voltage, e.g., by the controller of linear compressor 100. Any suitable time varying voltage may be supplied to the motor of linear compressor 100 at step 630. For example, the time varying voltage may have at least two frequencies components at step 630 when the electrical dynamic model for the motor of linear compressor 100 is solved for di/dt. Thus, the time varying voltage may be

v _(a)(t)=v ₀[sin(2πf ₁ t)+sin(2πf ₂ t)]

where

-   -   v_(a) is a voltage across the motor of linear compressor 100;     -   f₁ is a first frequency; and     -   f₂ is a second frequency.         The first and second frequencies f₁, f₂ may be about the         resonant frequency of linear compressor 100. In particular, the         first and second frequencies f₁, f₂ may be just greater than and         just less than the resonant frequency of linear compressor 100,         respectively. For example, the first frequency f₁ may be within         five percent greater than the resonant frequency of linear         compressor 100, and the second frequency f₂ may be within five         percent less than the resonant frequency of linear compressor         100. In alternative exemplary embodiments, the time varying         voltage may have a single frequency at step 630, e.g., when the         electrical dynamic model for the motor of linear compressor 100         is solved for {dot over (x)}. When the time varying voltage has         a single frequency at step 630, the gas force of fluid within         linear compressor 100 may be incorporated within the model for         the motor of linear compressor 100.

A time varying current through the motor of linear compressor 100 may also be determined, e.g., during step 630. An ammeter or any other suitable method or mechanism may be used to determine the time varying current through the motor of linear compressor 100. A velocity of the motor of linear compressor 100 may also be measured, e.g., during step 630. As an example, an optical sensor, a Hall effect sensor or any other suitable sensor may be positioned adjacent piston assembly 114 and/or inner back iron assembly 130 in order to permit such sensor to measure the velocity of the motor of linear compressor 100 at step 630. Thus, piston assembly 114 and/or inner back iron assembly 130 may be directly observed in order to measure the velocity of the motor of linear compressor 100 at step 630. In addition, a filtered first derivative of the current through the motor of linear compressor 100 with respect to time may also be measured or determined, e.g., during step 630. Accordingly, the values or filtered values of W may be measured during step 630. To permit such measuring, step 630 and the measurements described above may be conducted prior to sealing the motor of linear compressor 100 within a hermetic shell.

At step 640, an error between a measured variable (e.g., di/dt or k) of the electrical dynamic model at a first time and an estimated variable of the electrical dynamic model at the first time is calculated. For example, an estimate of θ_(e), {circumflex over (θ)}_(e), is available, e.g., from step 620. An error between θ_(e) and {circumflex over (θ)}_(e) may be given as

{tilde over (θ)}_(e)

θ_(e)−{circumflex over (θ)}_(e).

However, θ_(e) may be unknown while Φ_(f) is known or measured. Thus, a related error signal may be used at step 640. The related error signal may be given as

{tilde over (Φ)}_(f)

Φ_(f)−{circumflex over (Φ)}_(f).

The related error signal along with W_(f) may be used to update {circumflex over (θ)}_(e), as described in greater detail below.

At step 650, the estimate for each unknown constant of the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100 are repeatedly updated at each time after the first time in order to reduce the error between a measured variable of the electrical dynamic model at each time after the first time and an estimated variable of the electrical dynamic model at each time after the first time. In particular, an adaptive least-squares algorithm may be utilized in order to drive the error between the measured value for the electrical dynamic model at each time after the first time and the estimated variable of the electrical dynamic model at each time after the first time towards zero. In particular, the Adaptive Least-Squares Update Law ensures that

{tilde over (θ)}_(e)(t)→0 as t→∞:

${{\overset{.}{\hat{\theta}}}_{e}\overset{\Delta}{=}{{- k_{e}}\frac{P_{e}W_{f}^{T}{\overset{\sim}{\varphi}}_{f}}{1 + {\gamma_{e}W_{f}P_{e}W_{f}^{T}}}}},$

{circumflex over (θ)}_(e)(t₀) is estimated, e. g., at step 620.

where P_(e)(t)ε

^(3×3) is the covariance matrix

${{\overset{.}{P}}_{e}\overset{\Delta}{=}{{- k_{e}}\frac{P_{e}W_{f}^{T}W_{f}P_{e}}{1 + {\gamma_{e}W_{f}W_{f}^{T}}}}},{{P_{e}\left( t_{0} \right)} = {\rho_{e}I_{3}}}$

where k_(e), γ_(e), ρ_(e)ε

⁺ are constant gains.

From {circumflex over (θ)}_(e), estimates of each unknown constant of the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100 may be given as

${\hat{\alpha} = \frac{{\hat{\theta}}_{e_{3}}}{{\hat{\theta}}_{e_{1}}}},{\hat{R} = \frac{{\hat{\theta}}_{e_{2}}}{{\hat{\theta}}_{e_{1}}}},{\hat{L} = \frac{1}{{\hat{\theta}}_{e_{1}}}}$

when the electrical dynamic model for the motor of linear compressor 100 is solved for di/dt at step 610 or

${\hat{\alpha} = \frac{1}{{\hat{\theta}}_{e_{1}}}},{\hat{R} = \frac{{\hat{\theta}}_{e_{2}}}{{\hat{\theta}}_{e_{1}}}},{\hat{L} = \frac{{\hat{\theta}}_{e_{3}}}{{\hat{\theta}}_{e_{1}}}}$

when the electrical dynamic model for the motor of linear compressor 100 is solved for {dot over (x)} at step 610.

FIGS. 9, 10 and 11 illustrate exemplary plots of experimental electrical motor parameter estimates, e.g., taken during steps 640 and 650. As may be seen in FIGS. 9, 10 and 11, the initial estimate provided for the electrical motor parameters of linear compressor 100 may be off an actual or previously determined value. However, the experimental electrical motor parameter estimates converge to the previously determined values over time.

With the unknown constants of the electrical dynamic model for the motor of linear compressor 100 suitably estimated, a final estimate for each unknown constant of the plurality of unknown constants of the electrical dynamic model for the motor of linear compressor 100 may be saved within the controller of linear compressor 100. The saved constant values may be used to facilitate efficient and/or proper operation of linear compressor 100. In particular, knowledge of the constants of the electrical dynamic model for the motor of linear compressor 100 may assist with operating linear compressor 100 at a resonant frequency while avoiding head crashing.

As discussed above, method 600 may also provide estimates of the mechanical parameters or constants of linear compressor 100. Thus, method 600 may also include providing a mechanical dynamic model for linear compressor 100. Any suitable mechanical dynamic model for linear compressor 100 may be provided. For example, the mechanical dynamic model for linear compressor 100 may be

$F_{m} = {{i(t)} = {{\frac{M}{\alpha}\overset{¨}{x}} + {\frac{C}{\alpha}\overset{.}{x}} + {\frac{K}{\alpha}x}}}$

where

-   -   M is a moving mass of linear compressor 100;     -   α is a motor force constant;     -   {umlaut over (x)} is an acceleration of the motor of linear         compressor 100;     -   C is a damping coefficient of linear compressor 100;     -   {dot over (x)} is a velocity of the motor of linear compressor         100;     -   K is a spring stiffness of linear compressor 100; and     -   x is a position of the moving mass of linear compressor 100.

The mechanical dynamic model for linear compressor 100 includes a plurality of unknown constants. In the example provided above, the plurality of unknown constants of the mechanical dynamic model of linear compressor 100 includes a moving mass of linear compressor 100 (e.g., a mass of piston assembly 114 and inner back iron assembly 130), a damping coefficient of linear compressor 100, and a spring stiffness of linear compressor 100 (e.g., a stiffness of spring assembly 120). Knowledge or accurate estimates of such unknown constants can improve operation of linear compressor 100, e.g., by permitting operation of linear compressor 100 at a resonant frequency without head crashing.

The mechanical dynamic model for linear compressor 100 may also be solved for a particular variable, such as i(t) in the example provided above. Thus, as an example, the electrical dynamic model for the motor of linear compressor 100 may be provided in parametric form as

$\Psi \overset{\Delta}{=}{Y\; \theta_{m}}$ where ${\Psi \overset{\Delta}{=}\lbrack i\rbrack};$ ${Y\overset{\Delta}{=}\left\lbrack {\overset{¨}{x}\overset{.}{x}x} \right\rbrack};{and}$ $\theta_{m}\overset{\Delta}{=}{\left\lbrack {\frac{M}{\propto}\frac{C}{\propto}\frac{K}{\propto}} \right\rbrack^{T}.}$

However, {umlaut over (x)} is difficult to accurately measure or determine. Thus, a filtering technique may be used to account for this signal and provide a measurable variable. In particular, the mechanical dynamic model for linear compressor 100 may be filtered, e.g., with a low-pass filter, to account for this signal. Thus, a filtered electrical dynamic model for the motor of linear compressor 100 may be provided as

Ψ_(f)

Y _(f)θ_(m).

Each unknown constant of the plurality of unknown constants of the mechanical dynamic model for linear compressor 100 may also be estimated, and the motor (e.g., driving coil 152) of linear compressor 100 may be supplied with a time varying voltage, e.g., in the manner described above for steps 620 and 630.

An error between a measured variable of the mechanical dynamic model at the first time and an estimated variable of the mechanical dynamic model at the first time may also be calculated. For example, an estimate of θ_(m), {circumflex over (θ)}_(m), is available as discussed above. An error between θ_(m) and {circumflex over (θ)}_(m) may be given as

{tilde over (θ)}_(m)

θ_(m)−{circumflex over (θ)}_(m).

However, θ_(m) may be unknown while Ψ_(f) is known or measured. Thus, a related error signal may be used. The related error signal may be given as

{tilde over (Ψ)}_(f)

Ψ_(f)−{circumflex over (Ψ)}_(f).

The related error signal along with Y_(f) may be used to update {circumflex over (θ)}_(m), as described in greater detail below.

The estimate for each unknown constant of the plurality of unknown constants of the mechanical dynamic model for linear compressor 100 are repeatedly updated at each time after the first time in order to reduce the error between a measured variable of the mechanical dynamic model at each time after the first time and an estimated variable of the mechanical dynamic model at each time after the first time. In particular, an adaptive least-squares algorithm may be utilized in order to drive the error between the measured value for the mechanical dynamic model at each time after the first time and the estimated variable of the mechanical dynamic model at each time after the first time towards zero. In particular, the Adaptive Least-Squares Update Law ensures that

{tilde over (θ)}_(m)(t)→0 as t→∞:

${{\overset{.}{\hat{\theta}}}_{m}\overset{\Delta}{=}{{- k_{m}}\frac{P_{m}Y_{f}^{T}{\overset{\sim}{\Psi}}_{f}}{1 + {\gamma_{m}Y_{f}P_{m}Y_{f}^{T}}}}},$

{circumflex over (θ)}_(m)(t₀) is estimated.

where P_(m)(t)ε

^(3×3) is the covariance matrix

${{\overset{.}{P}}_{m}\overset{\Delta}{=}{{- k_{m}}\frac{P_{m}Y_{f}^{T}Y_{f}P_{m}}{1 + {\gamma_{m}Y_{f}Y_{f}^{T}}}}},{{P_{m}\left( t_{0} \right)} = {\rho_{m}I_{3}}}$

where k_(m), γ_(m), ρ_(m)ε

⁺ are constant gains.

From {circumflex over (θ)}_(m) and the estimate of the motor force constant from step 650, estimates of each unknown constant of the plurality of unknown constants of the mechanical dynamic model for linear compressor 100 may be given as

{circumflex over (M)}={circumflex over (α)}{circumflex over (θ)} _(m) ₁ ,Ĉ={circumflex over (α)}{circumflex over (θ)} _(m) ₂ ,{circumflex over (K)}={circumflex over (α)}{circumflex over (θ)} _(m) ₃ .

With the unknown constants of the mechanical dynamic model for linear compressor 100 suitably estimated, a final estimate for each unknown constant of the plurality of unknown constants of the mechanical dynamic model for linear compressor 100 may be saved within the controller of linear compressor 100. The saved constant values may be used to facilitate efficient and/or proper operation of linear compressor 100. In particular, knowledge of the constants of the mechanical dynamic model for linear compressor 100 may assist with operating linear compressor 100 at a resonant frequency while avoiding head crashing.

FIG. 7 illustrates a method 700 for operating a linear compressor according to another exemplary embodiment of the present subject matter. Method 700 may be used to operate any suitable linear compressor. For example, method 700 may be used to operate linear compressor 100 (FIG. 3). Thus, method 700 is discussed in greater detail below with reference to linear compressor 100. Utilizing method 700, a stroke length of the motor of linear compressor 100 may be established or determined. Knowledge of the stroke length of the motor of linear compressor 100 may improve performance or operation of linear compressor 100, as will be understood by those skilled in the art.

At step 710, an electrical dynamic model for the motor of linear compressor 100 is provided. Any suitable electrical dynamic model for the motor of linear compressor 100 may be provided at step 710. For example, the electrical dynamic model for the motor of linear compressor 100 described above for step 610 of method 600 may be used at step 710. The electrical dynamic model for the motor of linear compressor 100 may also be modified such that

$\frac{i}{t} = {\frac{v_{a}}{L_{i}} - \frac{r_{i}i}{L_{i}} - f}$ ${{where}\mspace{14mu} f} = {\frac{a}{L_{i}}{\overset{.}{x}.}}$

At step 720, the motor (e.g., driving coil 152) of linear compressor 100 is supplied with a time varying voltage, e.g., by the controller of linear compressor 100. Any suitable time varying voltage may be supplied to the motor of linear compressor 100 at step 720. As an example, the motor (e.g., driving coil 152) of linear compressor 100 may be supplied with a time varying voltage in the manner described above for step 630 of method 600. A time varying current through the motor of linear compressor 100 may also be determined, e.g., during step 720. An ammeter any other suitable method or mechanism may be used to determine the time varying current through the motor of linear compressor 100.

At step 730, a back-EMF of the motor of linear compressor 100 is estimated, e.g., during step 720. The back-EMF of the motor of linear compressor 100 may be estimated at step 730 using at least the electrical dynamic model for the motor of linear compressor 100 and a robust integral of the sign of the error feedback. As an example, the back-EMF of the motor of linear compressor 100 may be estimated at step 730 by solving

{circumflex over (f)}=(K ₁+1)e(t)+∫_(t) ₀ ^(t)[(K ₁+1)e(σ)+K ₂sgn(e(σ))]dσ−(K ₁+1)e(t ₀)

where

-   -   {circumflex over (f)} is an estimated back-EMF of the motor of         linear compressor 100;     -   K₁ and K₂ are real, positive gains; and     -   e=î−i and ė=f−{circumflex over (f)}; and     -   sgn is the signum or sign function.

At step 740, a velocity of the motor of linear compressor 100 is estimated. The velocity of the motor of linear compressor 100 may be estimated at step 740 based at least in part on the back-EMF of the motor from step 730. For example, the velocity of the motor of linear compressor 100 may be determined at step 740 by solving

$\hat{\overset{.}{x}} = {\frac{L_{i}}{\alpha}\hat{f}}$

where

-   -   {dot over ({circumflex over (x)})} is an estimated velocity of         the motor of linear compressor 100;     -   α is a motor force constant; and     -   L_(i) is an inductance of the motor of linear compressor 100.         The motor force constant and the inductance of the motor of         linear compressor 100 may be estimated with method 600, as         described above.

At step 750, a stroke length of the motor of linear compressor 100 is estimated. The stroke length of the motor of linear compressor 100 may be estimated at step 750 based at least in part on the velocity of the motor from step 740. In particular, the stroke length of the motor of linear compressor 100 may be estimated at step 750 by solving

$X = {{\frac{L_{i}}{\alpha}{\int{\hat{f}{t}}}} = {{\hat{x}}_{initial} + {\hat{x}(t)}}}$

where {circumflex over (x)} is an estimated position of the motor of linear compressor 100.

It should be understood that steps 720, 730, 740 and 750 may be performed with the motor of linear compressor 100 sealed within a hermitic shell of linear compressor 100. Thus, method 700 may be performed at any suitable time during operation of linear compressor 100 in order to determine the stroke length of the motor of linear compressor 100, e.g., because moving components of linear compressor 100 need not be directly measured with a sensor. Knowledge of the stroke length of the motor of linear compressor 100 may assist with operating linear compressor 100 efficiently and/or properly. For example, such knowledge may assist with adjusting the time varying voltage supplied to the motor of the linear compressor 100 in order to operate the motor of linear compressor 100 at a resonant frequency of the motor of linear compressor 100 without head crashing, etc., as will be understood by those skilled in the art.

FIG. 8 illustrates a method 800 for operating a linear compressor according to an additional exemplary embodiment of the present subject matter. Method 800 may be used to operate any suitable linear compressor. For example, method 800 may be used to operate linear compressor 100 (FIG. 3). Thus, method 800 is discussed in greater detail below with reference to linear compressor 100. Utilizing method 800, a position of the motor of linear compressor 100 when the motor of linear compressor 100 is at a top dead center point may be established or determined. Knowledge of the motor of linear compressor 100 at the top dead center point may improve performance or operation of linear compressor 100, as will be understood by those skilled in the art.

At step 810, a mechanical dynamic model for linear compressor 100 is provided. Any suitable mechanical dynamic model for linear compressor 100 may be provided. For example, the mechanical dynamic model for linear compressor 100 described above for method 600 may be used at step 810. As another example, the mechanical dynamic model for linear compressor 100 may be

F _(m) =αi=M{umlaut over (x)}+C{dot over (x)}+K(x _(avg) −x ₀)+F _(gas)

where

-   -   M is a moving mass of linear compressor 100;     -   α is a motor force constant;     -   {umlaut over (x)} is an acceleration of the motor of linear         compressor 100;     -   C is a damping coefficient of linear compressor 100;     -   {dot over (x)} is a velocity of the motor of linear compressor         100;     -   K is a spring stiffness of linear compressor 100;     -   x is a position of the moving mass of linear compressor 100; and     -   F_(gas) is a gas force.         Solving for acceleration, the mechanical dynamic model for         linear compressor 100 may be given as

$\overset{¨}{x} = {{{{- \frac{C}{M}}\overset{.}{x}} - {\frac{K}{M}\left( {x_{avg} - x_{0}} \right)} + {\frac{\alpha}{M}i} + {\frac{1}{M}F_{gas}}} = {{\frac{\alpha}{M}i} + {f_{x}(t)}}}$ where ${f_{x}(t)} = {{\frac{1}{M}F_{gas}} - {\frac{C}{M}\overset{.}{x}} - {\frac{K}{M}\left( {x_{avg} - x_{0}} \right)} + {\frac{\alpha}{M}{i.}}}$

At step 820, the motor (e.g., driving coil 152) of linear compressor 100 is supplied with a time varying voltage, e.g., by the controller of linear compressor 100. Any suitable time varying voltage may be supplied to the motor of linear compressor 100 at step 820. As an example, the motor (e.g., driving coil 152) of linear compressor 100 may be supplied with a time varying voltage in the manner described above for step 630 of method 600. At step 830, a time varying current through the motor of linear compressor 100 may also be determined, e.g., during step 820. In particular, a current to the motor of linear compressor 100 may be measured at step 830 when the motor of linear compressor 100 is at a bottom dead center point. Thus, a velocity of the motor of linear compressor 100 may be zero or about (e.g., within about a tenth of a meter per second) zero when the current to the motor of linear compressor 100 is measured at step 830. A voltmeter or any other suitable method or mechanism may be used to determine the current through the motor of linear compressor 100.

At step 840, an acceleration of the motor of linear compressor 100 is estimated, e.g., during step 820. The acceleration of the motor of linear compressor 100 may be estimated at step 840 using at least the mechanical dynamic model for linear compressor 100 and a robust integral of the sign of the error feedback. As an example, the acceleration of the motor of linear compressor 100 may be estimated at step 840 by solving

$\hat{\overset{¨}{x}} = {{\frac{\alpha}{M}i} + {{\hat{f}}_{x}(t)}}$

with {circumflex over (f)}_(x) being given as

{circumflex over (f)}=(k ₁+1)e _(x)(t)+∫_(t) ₀ ^(t)[(k ₁+1)e _(x)(σ)+k ₂sgn(e _(x)(σ))]dσ−(k ₁+1)e _(x)(t ₀)

and where

-   -   {umlaut over ({circumflex over (x)})} is an estimated         acceleration of the motor of linear compressor 100;     -   k₁ and k₂ are real, positive gains; and     -   e_(x)={dot over (x)}−{circumflex over ({dot over (x)})} and         s_(x)×ė_(x)+e_(x).

At step 850, a position of the motor of linear compressor 100 when the motor of the linear compressor 100 is at the bottom dead center point is determined. The position of the motor of linear compressor 100 when the motor of linear compressor 100 is at the bottom dead center point may be estimated at step 850 based at least in part on the current to the motor of linear compressor 100 from step 830 and the acceleration of the motor from step 840. For example, the position of the motor of linear compressor 100 when the motor of linear compressor 100 is at the bottom dead center point may be estimated at step 850 by solving

$x_{BDC} = {{\frac{\alpha}{K}i_{BDC}} - {\frac{M}{K}{\overset{¨}{x}}_{BDC}}}$

where

-   -   α is a motor force constant;     -   K is a spring stiffness of linear compressor 100;     -   i_(BDC) is the current to the motor of linear compressor 100 at         the bottom dead center point;     -   M is a moving mass of linear compressor 100; and     -   {umlaut over (x)}_(BDC) is the acceleration of the motor at the         bottom dead center point. The motor force constant, the spring         stiffness of linear compressor 100 and the moving mass of linear         compressor 100 may be estimated with method 600, as described         above.         At step 860, a position of the motor of linear compressor 100         when the motor of linear compressor 100 is at the top dead         center point is determined. The position of the motor of linear         compressor 100 when the motor of linear compressor 100 is at the         top dead center point may be estimated at step 860 based at         least in part on the position of the motor of linear compressor         100 when the motor of linear compressor 100 is at the bottom         dead center point from step 850 and a stroke length of the motor         of linear compressor 100. For example, the position of the motor         of linear compressor 100 when the motor of linear compressor 100         is at the top dead center point may be estimated at step 860 by         solving

x _(TDC) =x _(BDC)−SL

where SL is the stroke length of the motor of linear compressor 100.

The stroke length of the motor of linear compressor 100 may be estimated with method 700, as described above.

It should be understood that steps 820, 830, 840, 850 and 860 may be performed with the motor of linear compressor 100 sealed within a hermitic shell of linear compressor 100. Thus, method 800 may be performed at any suitable time during operation of linear compressor 100 in order to determine the position of the motor of linear compressor 100 when the motor of linear compressor 100 is at the top dead center point, e.g., because moving components of linear compressor 100 need not be directly measured with a sensor. Knowledge of the position of the motor of linear compressor 100 when the motor of linear compressor 100 is at the top dead center point may assist with operating linear compressor 100 efficiently and/or properly. For example, such knowledge may assist with adjusting the time varying voltage supplied to the motor of the linear compressor 100 in order to operate the motor of linear compressor 100 at a resonant frequency of the motor of linear compressor 100 without head crashing, etc., as will be understood by those skilled in the art.

This written description uses examples to disclose the invention, including the best mode, and also to enable any person skilled in the art to practice the invention, including making and using any devices or systems and performing any incorporated methods. The patentable scope of the invention is defined by the claims, and may include other examples that occur to those skilled in the art. Such other examples are intended to be within the scope of the claims if they include structural elements that do not differ from the literal language of the claims, or if they include equivalent structural elements with insubstantial differences from the literal languages of the claims. 

What is claimed is:
 1. A method for operating a linear compressor, comprising: providing an electrical dynamic model for a motor of the linear compressor; supplying the motor of the linear compressor with a time varying voltage; estimating a back-EMF of the motor of the linear compressor during said step of supplying using at least the electrical dynamic model for the motor of the linear compressor and a robust integral of the sign of the error feedback; determining a velocity of the motor of the linear compressor based at least in part on the back-EMF of the motor from said step of estimating; and calculating a stroke length of the motor of the linear compressor based at least in part on the velocity of the motor from said step of determining.
 2. The method of claim 1, wherein the electrical dynamic model for the motor comprises $\frac{i}{t} = {\frac{v_{a}}{L_{i}} - \frac{r_{i}i}{L_{i}} - \frac{\alpha \; \overset{.}{x}}{L_{i}}}$ where v_(a) is a voltage across the motor of the linear compressor; r_(i) is a resistance of the motor of the linear compressor; i is a current through the motor of the linear compressor; α is a motor force constant; {dot over (x)} is a velocity of the motor of the linear compressor; and L_(i) is an inductance of the motor of the linear compressor.
 3. The method of claim 2, further establishing a time varying current through the motor of the linear compressor during said step of supplying.
 4. The method of claim 1, wherein the linear compressor is positioned within a refrigerator appliance.
 5. The method of claim 1, wherein estimating the back-EMF of the motor of the linear compressor during said step of supplying using the robust integral of the sign of the error feedback comprises solving {circumflex over (f)}=(K ₁+1)e(t)+∫_(t) ₀ ^(t)[(K ₁+1)e(σ)+K ₂sgn(e(σ))]dσ−(K ₁+1)e(t ₀) where {circumflex over (f)} is an estimated back-EMF of the motor of the linear compressor; K₁ and K₂ are real, positive gains; and e=î−i and ė=f−{circumflex over (f)}.
 6. The method of claim 5, said step of determining the velocity of the motor of the linear compressor comprises solving $\hat{\overset{.}{x}} = {\frac{L_{i}}{\alpha}\hat{f}}$ where {dot over ({circumflex over (x)})} is an estimated velocity of the motor of the linear compressor; α is a motor force constant; and L_(i) is an inductance of the motor of the linear compressor.
 7. The method of claim 6, wherein said step of calculating the stroke length of the motor of the linear compressor comprises solving $X = {{\frac{L_{i}}{\alpha}{\int{\hat{f}{t}}}} = {{\hat{x}}_{initial} + {\hat{x}(t)}}}$ where {circumflex over (x)} is an estimated position of the motor of the linear compressor.
 8. The method of claim 1, further comprising adjusting the time varying voltage supplied to the motor of the linear compressor in order to operate the motor of the linear compressor at a resonant frequency of the motor of the linear compressor.
 9. The method of claim 1, wherein said steps of estimating, determining and calculating are conducted with the motor of the linear compressor sealed within a hermitic shell of the linear compressor.
 10. A method for operating a linear compressor, comprising: supplying the motor of the linear compressor with a time varying voltage, the motor of the linear compressor disposed within a hermetic shell of the linear compressor during said step of supplying; estimating a back-EMF of the motor of the linear compressor during said step of supplying using a robust integral of the sign of the error feedback; determining a velocity of the motor of the linear compressor based at least in part on the back-EMF of the motor from said step of estimating; and calculating a stroke length of the motor of the linear compressor based at least in part on the velocity of the motor from said step of determining.
 11. The method of claim 10, further comprising providing an electrical dynamic model for the motor of the linear compressor, the electrical dynamic model for the motor comprising $\frac{i}{t} = {\frac{v_{a}}{L_{i}} - \frac{r_{i}i}{L_{i}} - \frac{\alpha \; \overset{.}{x}}{L_{i}}}$ where v_(a) is a voltage across the motor of the linear compressor; r_(i) is a resistance of the motor of the linear compressor; i is a current through the motor of the linear compressor; α is a motor force constant; {dot over (x)} is a velocity of the motor of the linear compressor; and L_(i) is an inductance of the motor of the linear compressor.
 12. The method of claim 11, further establishing a time varying current through the motor of the linear compressor during said step of supplying.
 13. The method of claim 11, the linear compressor is positioned within a refrigerator appliance.
 14. The method of claim 10, wherein estimating the back-EMF of the motor of the linear compressor during said step of supplying using the robust integral of the sign of the error feedback comprises solving {circumflex over (f)}=(K ₁+1)e(t)+∫_(t) ₀ ^(t)[(K ₁+1)e(σ)+K ₂sgn(e(σ))]dσ−(K ₁+1)e(t ₀) where {circumflex over (f)} is an estimated back-EMF of the motor of the linear compressor; K₁ and K₂ are real, positive gains; and e=î−i and e=f−{circumflex over (f)}.
 15. The method of claim 14, said step of determining the velocity of the motor of the linear compressor comprises solving $\hat{\overset{.}{x}} = {\frac{L_{i}}{\alpha}\hat{f}}$ where {dot over ({circumflex over (x)})} is an estimated velocity of the motor of the linear compressor; α is a motor force constant; and L_(i) is an inductance of the motor of the linear compressor.
 16. The method of claim 15, wherein said step of calculating the stroke length of the motor of the linear compressor comprises solving $X = {{\frac{L_{i}}{\alpha}{\int{\hat{f}{t}}}} = {{\hat{x}}_{initial} + {\hat{x}(t)}}}$ where {circumflex over (x)} is an estimated position of the motor of the linear compressor.
 17. The method of claim 10, further comprising adjusting the time varying voltage supplied to the motor of the linear compressor in order to operate the motor of the linear compressor at a resonant frequency of the motor of the linear compressor. 